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Stellar Structure Evolution
VO• CS: show peculiar absorption lines in their spectra• They are NOT grouped in early- solar and late-type according to their ageYerks spectral classification: two-dimensional system. It’s a luminosity-based class. Classificationwas based on the visual inspection of strong lines: the rate of ionisation is essentially determinedby the radiation field hence more luminous stars have deeper lines.
Lesson 10: Stellar structure evolutionWe will assume that a star is a huge sphere of gas without rotation, magnetic field or mass loss.+/- all stars are made of: end of their life.2 FORCES:• Gravity: pulls the stellar material towards the centre. Confines the gas in the star againstpressure expansion.• Pressure: due to thermal motions of the gas molecules tends to expand the gas outward.Support the star against gravitational collapseBalance everywhere -> hydrostatic equilibriumWRONG: Hydrostatic equilibrium is naturally realized without requiring any source of
energy
Free-fall timescale: time required for a star to collapse to a point if there is no outward pressure to counteract gravity
Kevin Helmholtz
time it takes for the object to radiate away a significant amount of its gravitational potential energy
Nuclear time scale
time to radiate the energy produced by the mass difference between the reactants and product of the nuclear reaction.
The mass of the nucleus is smaller than the sum of the masses of all its nucleons. The difference is called "binding energy per nucleon".
Radiation
energy transfer in the form of electromagnetic radiation
Convection
starts when radiation becomes inefficient I.e. photons cannot travel freely
Conduction
in stars is very inefficient, because electrons can travel only short distance
Vogt-Russell Theorem
the structure of a star, in hydrostatic and thermal equilibrium with all energy derived from nuclear reaction is uniquely determined by its MASS and the distribution of chemical elements throughout
point, the central temperature and pressure become high enough for nuclear fusion to start in thecore. The protostar becomes a main sequence star.The hydrostatic equilibrium settles in during the protostar phase. The central temperature is too low for H fusion but enough for Li and deuterium burning.
Even the smallest perturbation can start a rotation motion in the cloud. For conservation of angular momentum, the cloud will become ellipsoidal, and the gravity of the thicker part will shape it as a disk.
Herbig-Haro objects are characterized by the expulsion of partially ionized gas on narrow jets, perpendicular to the accretion disk.
Energy is provided by hydrogen fusion in the core through PP-chains.
- Stars have greater gravitational compression in their cores with increasing mass.
- Greater thermal and radiation pressure is required to balance the greater gravitational compression.
- The greater thermal pressure is provided by higher temperatures in the stellar core. Massive stars need higher core temperatures to be stable.
- Higher energy production in the core means that more energy will leave the surface. Energy cannot be stored inside the star. Luminosity increases with mass.
- Object with masses smaller than 0.08 solar masses are not massive enough to start Hydrogen Fusion
- The energy sustain the hydrodynamical equilibrium is provided by Hydrogen fusion in the core
- Stars more massive than 120 solar masses are predicted to be unstable, although exceptions have been observed
- WRONG: In the colour magnitude diagram, Main Sequence stars are randomly scattered all across the diagram
- Chemical reaction or radioactivity are not efficient enough to justify the luminosity of the sun
- By radiating its gravitational potential energy a star could survive a few million years
- WRONG: Without any internal pressure to counterbalance gravity, a star would collapse in 15 minutes.
- WRONG: Nuclear reactions keep a star shining for billions of years.
star in balance for billions of years only if all its mass inconverted to energy
Carbon burning phase and beyond in stellar evolution
- After carbon ignition, the star goes through a series of alternating nuclear burning/corecontraction cycles
- Each nuclear burning phase is much quicker than the previous one, with silicon-burninglasting only few weeks
- Carbon fusion in the core starts if the Carbon-Oxygen core has a mass greater thansolar masses1.06
- WRONG: neutrino losses play only a minor contribution to the energy loss of the star, sincethey don't have any mass
Giant phase in stellar evolution:
- The turn-off is the point in the colour magnitude diagram where the star leaves the MainSequence to enter the giant phase
- When hydrogen is exhausted in the core, the star starts burning it in a shell surrounding aninert Helium core
- Giant stars are colder on the surface, but they are brighter because they have a largersurface than main sequence
Stars in the giant phase have the same size and luminosity, regardless of their mass during the main sequence phase
Asymptotic giant phase in stellar evolution (intermediate mass-stars)
- When helium in the core is exhausted, helium keeps burning in a shell leaving behind a carbon and oxygen core
- The star becomes unstable due to the presence of two shells with fusion reactions, Hydrogen and Helium respectively
- The star will lose the outer envelope into space, the expelled material takes the name of planetary nebula
- WRONG: the outcome of this phase will be a white dwarf either made of carbon and oxygen or just exclusively helium
Helium burning phase in stellar evolution (massive stars)
- Wolf-Rayet stars are exposed Hydrogen- or Helium-burning cores of massive stars, often surrounded by ejected material
- The Humphreys-Davidson limit sets the maximum luminosity of a star before becoming unstable for radiation pressure
- Luminous blue variables
energy• WRONG: Neutronization and photo-disintegration increase the pressure in the core, slowing down the collapse
Lesson 11: Compact objects (low and medium-mass stars)
Normal gas:• thermal effects dominate, increasing the temperature will increase the pressure. When two atoms approach each other, the electrons in one atom repel the electrons in the other atom via electric forces.
• Under high densities the gas becomes a collection of positively charged ions floating in a sea of electrons, which have been stripped from the nuclei. The electron degeneracy pressure is independent of temperature because it is related to the repulsive force.
• At even higher density, electrons and protons merge together to form a neutron sea. The neutron degeneracy pressure is similar to the E.D.P but it is stronger.
White dwarf: when there is no nuclear reaction in the core, density increases until the gas becomes a collection of positively charged ions floating in a sea of electrons which have
Il testo formattato con i tag HTML è il seguente:Been stripped from the nuclei. Compression does not lead to heating and expansion as in regular stars: . Temperature does not depend on density. WDS are hot because of previous stages of stellar evolution not because of their degenerate status.
Other characteristics:
- Mainly composed by O and C, with a thin H and He atmosphere
- Initially hot but they are "dim" (low luminosity) because of small size
- No source of energy, they will gradually cool and become black dwarfs
- When cools down, carbon assumes a crystalline configuration similar to those of diamonds
- Matter forms an accretion disk around the WD and eventually fall on it
- Compression does not lead to heating an expansion as in regular stars: increases the mass causes smaller radius